L 2 -transforms for boundary value problems
|
|
- Byron Chandler
- 5 years ago
- Views:
Transcription
1 Computational Method for Differential Equation Vol. 6, No., 8, pp L -tranform for boundary value problem Arman Aghili Department of applied mathematic, faculty of mathematical cience, Univerity of Guilan, Raht-Iran, P. O. Box arman.aghili@gmail.com Abtract In thi article, we will how the complex inverion formula for the inverion of the L -tranform and alo ome application of the L, and Pot-Widder tranform for olving ingular integral equation with trigonometric kernel. Finally, we obtained analytic olution for a partial differential equation with non-contant coefficient. Keyword. Laplace tranform, L -tranform, Pot-Widder tranform, Singular integral equation. Mathematic Subject Claification. 6A33, 44A, 44A, 35A.. Introduction The integral tranform receive a pecial attention in the literature becaue of it different application and therefore i conidered a a tandard technique in olving partial differential equation and ingular integral equation. The integral tranform technique i one of the mot ueful tool of applied mathematic employed in many branche of cience and engineering. The Laplace-type integral tranform called the L -tranform wa introduced by Yurekli [5] and denoted a follow L {f(t; } = te t f(tdt. (. Like the Fourier and Laplace tranform, the L, i ued in a variety of application. Perhap the mot common uage of the L -tranform i in the olution of initial value problem. Many problem of mathematical interet lead to the L -tranform whoe invere are not readily expreed in term of tabulated function. For the abence of method for inverion of the L -tranform, recently the author [, 3], etablihed a imple formula to invert the L -tranform of a deired function. In thi tudy, we preent ome new inverion technique for the L -tranform and an application of generalized product theorem for olving ome ingular integral equation and boundary value problem. Contructive example are alo provided. Example.. Let u verify the following identity L {δ(t k λ; } = e k kλ λ Received: 6 June 7 ; Accepted: 6 March 8. kλ k, λ >, k >. (. λ 76
2 CMDE Vol. 6, No., 8, pp Solution. By definition of the L -tranform, we have L {δ(t k λ; } = + te t δ(t k λdt. (.3 Let u introduce a change of variable t k λ = ξ, then we get L {δ(t k λ; } = + k e ξ + λ k(ξ+λ k ξ+λ δ(ξ uing elementary property of Dirac delta function, we arrive at L {δ(t k λ; } = e kλ k λ dξ k(ξ + λ k ξ + λ, (.4 kλ k λ. (.5. Elementary Propertie of the L -Tranform In thi ection, we recall ome propertie of the L -tranform that will be ueful to olve partial differential equation. The real merit of the L -tranform i revealed by it effect on derivative. Here we will derive a relation between the L -tranform of the derivative of the function and the L -tranform of the function itelf. Firt, we tate a Lemma about the L -tranform of δ-derivative. Lemma.. If f, f,..., f (n are all continuou function with a piecewie continuou derivative f (n on the interval t and if all function are of exponential order exp(c t a t for ome real contant c then ( For n =,,... L {δ n t f(t; } = n n L {f(t; } n (n f( + (. ( For n =,,... n (n (δ t f( + (δ n t f( +. L {t n f(t; } = ( n n δn L {f(t; }, (. where the differential operator δ t, δ t, are defined a below δ t = t Proof. See [5]. d dt, δ t = δ t δ t = d t dt d t 3 dt. 3. Complex Inverion Formula for the L -Tranform and Efro Theorem Lemma 3.. Let F ( be analytic function (auming that = i not a branch point except at finite number of pole each of which lie to the left hand ide of the
3 78 A. AGHILI vertical line Re = c and if F ( a through the left plane Re c, and then L {f(t; } = L {F (} = f(t = πi t exp( t f(tdt = F (, (3. F ( e t d = m [Re{F ( e t }, = k ]. k= (3. Proof. See [, ]. Example 3.. Let u olve the following impulive differential equation with noncontant coefficient. t y (t + λy(t = t β δ(t ξ, y( =. (3.3 Solution. The impule function i a ueful concept in a wide variety of mathematical phyic problem involving the idea impulive force or point ource. By taking the L -tranform of the above equation term wie, we get L (δ t y(t + λl (y(t = L (t β δ(t ξ. (3.4 Let u aume that L (y(t = Y (, then after evaluation of the L -tranform each term, we arrive at Y ( + λy ( = ξ β+ e ξ, (3.5 olving the above equation, lead to Y ( = ξβ+ e ξ + λ, (3.6 uing complex inverion formula for the L -tranform, we obtain y(t = πi ( ξβ+ e ξ + λ et d, (3.7 at thi point, direct application of the econd part of the Lemma (. lead to the following olution y(t = ξ β+ e (ξ t λ. (3.8 Lemma 3.. Efro Theorem for L -Tranform Let L (f(t = F ( and auming Φ(, q( are analytic and uch that, L (Φ(t, τ = Φ(τe τ q (, then we have the following { } L f(τφ(t, τd τ = F (q(φ(. (3.9 Proof. By definition of the L -tranform L { f(τφ(t, τdτ} = te t ( f(τφ(t, τdτdt, (3.
4 CMDE Vol. 6, No., 8, pp and changing the order of integration we arrive at f(τ( te t φ(t, τdtdτ = Φ( f(ττe τ q ( dτ = Φ(F (q(. Example 3.. Let u olve the following ingular integral equation (3. f(τ τ co(tτdτ = t ( ν. (3. Solution. Differentiating with repect to t on the both ide of the above relation, lead to f(τ in(tτdτ = ( νt ν, (3.3 τ and applying the L -tranform followed by the generalized product theorem and uing the fact that L {in(τt} = π τ 4 3 τe 4, (3.4 and L [x ν, x > ] = Γ( ν + ν+, (3.5 we arrive at or F ( π 3 ν ( νγ( = 43 3 ν, (3.6 F ( = ( νγ( 3 ν π4ν ν, (3.7 finally by inverion of the L -tranform we get 3 ν ( νγ( f(t = π4ν Γ(ν t (ν. (3.8 In the next ection, we give ome illutrative example and Lemma related to the L, Pot-Widder tranform, and complex inverion formula for the Pot-Widder tranform. 4. Illutrative Lemma and Example Lemma 4.. By uing complex inverion formula for the L -tranform, we can how that ξ J (tξ t( + ξ dξ = t K (t = t (t (t u e 4u du u, (4.
5 8 A. AGHILI where K i the modified Beel function of order one, with the above integral repreentation. Proof. It i well known that L [L (φ(x; x > p]p > ] = P(φ(x; x >, (4. therefore, the left hand ide of (4. can be written a follow L [L ( ξj (tξ t ; ξ > p]p > ] = P(ξJ (tξ ; ξ >. (4.3 t Applying the L -tranform two time on ( ξ t J (tξ and uing the fact that we get L {( ξ t t J (tξ} = e 4 P( ξj (tξ t 4, (4.4 t ; ξ > = L [ e 4p p 4 ]p > ] = t pe p e 4p dp. (4.5 p4 At thi point, let u intrduce a change of variable u = p, after implifying we obtain P( ξj (tξ ; ξ > = t t (t e u t 4u du u = t K (t. (4.6 Lemma 4.. Show that the following ingular integral equation of Pot-Widder type + ug(u u + du = a + b, (4.7 ha a formal olution a below 4a g(u = π a u b. (4.8 Proof. By definition of the invere Pot-Widder tranform we have g(u = ( c+i c +i e p e u dp d, (4.9 πi πi ap + b c i > introducing the new variable w = ap + b lead to g(u = ( c+i δ+i e w( e u a b a dw πi πi w = πi δ i ( ( e u a Γ( e b a d, > d (4.
6 CMDE Vol. 6, No., 8, pp hence g(u = πi therefore, the final olution i a below g(u = 4 a Γ(. Γ(. u b a e (u b a 4 a. Γ( d = 4 ( a Γ( πi = e (u b a d, (4. 4a π au b. (4. Lemma 4.3. Show that the following Pot-Widder type ingular integral equation + uφ(u u + du = ln a k λ, (4.3 ha a olution a below φ(u = au k + λ. (4.4 Proof. We may ue the following inverion formula for Pot-Widder tranform [] P {F (} = πi {F (u e iπ F (u e iπ }. (4.5 By uing the above inverion formula for Pot-Widder tranform, we obtain P { ln a k λ } = πi { ln(u e iπ a(u e iπ k λ ln(u e iπ = πi { ln u iπ au k λ a(u e iπ k λ } ln u+iπ au k λ } = au k +λ. Example 4.. Let u olve the following homogeneou ingular integral equation π f(τ in(tτ dτ = t ν. (4.6 Solution. The L -tranform of the above integral equation, lead to the following or F ( = F ( π ν Γ( + = 43 3 ν+, (4.7 5 ν Γ( ν ν f(t = L [ Γ( 5 ν ν Γ(ν ν ] f(t = Γ( 5 ν ν Γ(νt ν. Example 4.. By uing complex inverion formula for L -tranform, we how that [ ] L λ exp (n+ 4 = ( t λ n I n (λt, (4.8 where I n (. i the modified Beel function of the firt kind of order n. Solution. Let ( λ F ( = exp (n+ 4, (4.9
7 8 A. AGHILI then, we have F ( = exp(λ. (4. n+ 4 Therefore, = i a ingular point (eential ingularity not branch point. After uing the above complex inverion formula, we obtain the original function a following { ( } λ f(t = Re exp exp(t, = b n+, (4. 4 where, b i the coefficient of the term in the Laurent expanion of F ( exp(t. Therefore we get the following relation or F ( exp(t = F ( exp(t = [ ] [ ] + (t + (t n+! (4! + (4 3 3! +, (4. ] [ ] [ + (t (t n n! + (t n+ (n+! + λ n 4 + λ4 n+ 4 n+! + λ6 4 3 n+3 3! +, from the above expanion we obtain [ f(t = b = n! + (λt 4 (n +!! + (λt 4 4 (n +!! + (λt 6 ] 4 3 (n + 3!3! + t n. f(t = tn λ n k= (4.3 (λt k+n k (n + k!k!, (4.4 by uing erie expanion for the modified Beel function, we get the following f(t = b = ( t λ n I n (λt. (4.5 Example 4.3. Let u olve the following ingular integral equation with trigonometric kernel xφ(x co ξxdx = e ξ Erfc( ξ. (4.6 Solution. Taking the Laplace tranform of both ide of the integral equation with repect to λ, we get L{ xφ(x co λxdx} = (, (4.7
8 CMDE Vol. 6, No., 8, pp or, equivalently x x + φ(xdx = (, (4.8 the left hand ide of the above relation i Widder potential tranform of φ(x [4]. we obtain P{φ(x; } = (, (4.9 or φ(x = πi ( x e iπ (x e iπ x e iπ x e iπ (x e iπ, (4.3 x eiπ after implifying, we get π φ(x = x 3 (x +. (4.3 Lemma 4.4. The following identity hold true L +λ π {e x ( + λ } = x e 4t Erf(. (4.3 t + t Proof. By etting F ( = e x +λ ( +λ we have F ( +λ = e x +λ. In order to avoid complex integration along complicated key-hole contour, we may ue an appropriate integral repreentation for e ξ a follow e ξ = e η ξ 4η dη, (4.33 π if we ubtitute ξ = x + λ in the above integral, we get f(x, t = πi e x +λ +λ e t d ( = c+i πi +λ e η x (+λ 4η dη e t d = e (η +λt ( πi e (η +λt e (x 4η t (+λ 4η +λ d dη. Let u make a change of variable w = + λ to get f(x, t = c +i πi By uing the fact that, L { e a integral, we finally get f(x, t = c i e (x 4η t w 4η w dw dη. } = H(t a and etting a = x 4η t in the inner e (η +λt H(t x 4η t 4η dη = π e 4t x Erf( t + t. (4.34
9 84 A. AGHILI In the next ection, we implemented the L -tranform for olving partial differential equation. 5. The L -Tranform For Boundary Value Problem The econd order partial differential equation with non-contant coefficient have a number of application in electrical and mechanical engineering, medical cience and economic. Thi ection i devoted to the application of uch PDE. Problem 5.. Let u olve the following parabolic type partial differential equation t u t + u rr + r u r = λ u, < r <, t >, (5. with boundary condition u(, t = β exp( λ t, u(r, = T, u(r, t < M, where T, M are poitive contant. Solution. Let u take the L -tranform of the above equation term wie, we get or ( + λ U(r,.5u(r, + U rr (r, + r U r(r, =, (5. U rr + r U r + ( + λ U = T, U(, = ( β/( + λ, U(r, < M. (5.3 The general olution of the tranformed equation i given in term of the Beel function a below U(r, = c J (r + λ + c Y (r + λ + T + λ, (5.4 ince, Y (r i unbounded a r, we have to chooe c =, thu U(r, = c J (r + λ + T + λ, (5.5 β T +β ( +λ J, ( +λ from U(, = +λ, we find c = therefore U(r, = T + λ (T + βj (r + λ ( + λ J ( + λ. (5.6 By uing complex inverion formula for the L -tranform, we get u(r, t = T e λ t (T + β πi c+ e t J ( + λ r ( + λ J ( d, (5.7 + λ the integrand in the above integral ha imple pole at + λ = η n, n =,, 3,... and alo at + λ = where η n are imple zero of Beel function a + λ = η, η,..., η n,,..., hence, we deduce that the reidue of integrand at = λ i lim λ ( + e t J ( + λ λ r ( + λ J ( + λ = e λ t, (5.8
10 CMDE Vol. 6, No., 8, pp and alo reidue of integrand at = η n λ i lim +ηn λ( + λ ηn e t J ( + λ r ( + λ J ( + λ = ( + λ η ( n = lim +ηn λ J ( e t J ( + λ lim r + λ +ηn + λ λ = ( ( e η n t J (η n r = lim +ηn λ J ( + λ η = e η n t J (η n r. +λ n η n J (η n Where we have ued L Hopital rule in evaluating the limit and alo the fact that J (u = J (u, then u(r, t = T e λ t (T + β{e λ t e η n t J (η n r } =... η n J (η n u(r, t = 4(T + β n= e η n t J (η n r η n J (η n 6. Concluion n= βλe λ t. (5.9 The main purpoe of the preent tudy i to extend the application of the L - tranform to derive an analytic olution of boundary value problem. We have preented a method for olving ingular integral equation and boundary value problem uing the L -tranform and it i hoped that thee reult and other derived from thi be ueful to reearcher in the variou branche of the integral tranform and applied mathematic. 7. Acknowledgment The author would like to thank the anonymou referee/ and editor/ for careful and thoughtful reading of the manucript and ueful uggetion which helped to improve the preentation of the reult. Reference [] A. Aghili, A. Anari, Solving partial fractional differential equation uing the L A - tranform, Aian- European Journal of Mathematic, 3( (, 9. [] A. Aghili, A note on Fox-ingular integral equation and it application, Int. J. Contemp. Math. Science, (8 (7, [3] A. Aghili, A. Anari, and A. Sedghi, An inverion technique for the L - tranform with application, Int. J. Contemp. Math. Science, (8 (7, [4] A. Aghili, A. Anari, New method for olving ytem of P. F. D. E. and fractional evolution diturbance equation of ditributed order, Journal of Interdiciplinary Mathematic, April. [5] O. Yurekli, I. Sadek, A Pareval-Goldtein type theorem on the widder potential tranform and it application, International Journal of Mathematic and Mathematical Science, 4(3 (99,
Chapter 4. The Laplace Transform Method
Chapter 4. The Laplace Tranform Method The Laplace Tranform i a tranformation, meaning that it change a function into a new function. Actually, it i a linear tranformation, becaue it convert a linear combination
More informationNon-homogeneous time fractional heat equation
33 JACM 3, No., 33-4 (8) Journal of Abtract and Computational Mathematic http://www.ntmci.com/jacm Non-homogeneou time fractional heat equation A. Aghili Department of Applied Mathematic, Faculty of Mathematical
More informationReading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions
Chapter 4 Laplace Tranform 4 Introduction Reading aignment: In thi chapter we will cover Section 4 45 4 Definition and the Laplace tranform of imple function Given f, a function of time, with value f(t
More informationReading assignment: In this chapter we will cover Sections Definition and the Laplace transform of simple functions
Chapter 4 Laplace Tranform 4 Introduction Reading aignment: In thi chapter we will cover Section 4 45 4 Definition and the Laplace tranform of imple function Given f, a function of time, with value f(t
More informationSECTION x2 x > 0, t > 0, (8.19a)
SECTION 8.5 433 8.5 Application of aplace Tranform to Partial Differential Equation In Section 8.2 and 8.3 we illutrated the effective ue of aplace tranform in olving ordinary differential equation. The
More informationThe Power Series Expansion on a Bulge Heaviside Step Function
Applied Mathematical Science, Vol 9, 05, no 3, 5-9 HIKARI Ltd, wwwm-hikaricom http://dxdoiorg/0988/am054009 The Power Serie Expanion on a Bulge Heaviide Step Function P Haara and S Pothat Department of
More informationLecture 17: Analytic Functions and Integrals (See Chapter 14 in Boas)
Lecture 7: Analytic Function and Integral (See Chapter 4 in Boa) Thi i a good point to take a brief detour and expand on our previou dicuion of complex variable and complex function of complex variable.
More informationBogoliubov Transformation in Classical Mechanics
Bogoliubov Tranformation in Claical Mechanic Canonical Tranformation Suppoe we have a et of complex canonical variable, {a j }, and would like to conider another et of variable, {b }, b b ({a j }). How
More informationLaplace Transformation
Univerity of Technology Electromechanical Department Energy Branch Advance Mathematic Laplace Tranformation nd Cla Lecture 6 Page of 7 Laplace Tranformation Definition Suppoe that f(t) i a piecewie continuou
More information7.2 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 281
72 INVERSE TRANSFORMS AND TRANSFORMS OF DERIVATIVES 28 and i 2 Show how Euler formula (page 33) can then be ued to deduce the reult a ( a) 2 b 2 {e at co bt} {e at in bt} b ( a) 2 b 2 5 Under what condition
More informationIntroduction to Laplace Transform Techniques in Circuit Analysis
Unit 6 Introduction to Laplace Tranform Technique in Circuit Analyi In thi unit we conider the application of Laplace Tranform to circuit analyi. A relevant dicuion of the one-ided Laplace tranform i found
More informationApproximate Analytical Solution for Quadratic Riccati Differential Equation
Iranian J. of Numerical Analyi and Optimization Vol 3, No. 2, 2013), pp 21-31 Approximate Analytical Solution for Quadratic Riccati Differential Equation H. Aminikhah Abtract In thi paper, we introduce
More informationCHE302 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang
CHE3 ECTURE V APACE TRANSFORM AND TRANSFER FUNCTION Profeor Dae Ryook Yang Fall Dept. of Chemical and Biological Engineering Korea Univerity CHE3 Proce Dynamic and Control Korea Univerity 5- SOUTION OF
More informationAN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE TRANSFORM
Journal of Inequalitie Special Function ISSN: 7-433, URL: http://www.iliria.com Volume 6 Iue 5, Page 5-3. AN EXAMPLE FOR THE GENERALIZATION OF THE INTEGRATION OF SPECIAL FUNCTIONS BY USING THE LAPLACE
More informationLaplace Adomian Decomposition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernels
Studie in Nonlinear Science (4): 9-4, ISSN -9 IDOSI Publication, Laplace Adomian Decompoition Method for Solving the Nonlinear Volterra Integral Equation with Weakly Kernel F.A. Hendi Department of Mathematic
More informationAnalysis of Step Response, Impulse and Ramp Response in the Continuous Stirred Tank Reactor System
ISSN: 454-50 Volume 0 - Iue 05 May 07 PP. 7-78 Analyi of Step Repone, Impule and Ramp Repone in the ontinuou Stirred Tank Reactor Sytem * Zohreh Khohraftar, Pirouz Derakhhi, (Department of hemitry, Science
More informationApplication of Laplace Adomian Decomposition Method on Linear and Nonlinear System of PDEs
Applied Mathematical Science, Vol. 5, 2011, no. 27, 1307-1315 Application of Laplace Adomian Decompoition Method on Linear and Nonlinear Sytem of PDE Jaem Fadaei Mathematic Department, Shahid Bahonar Univerity
More informationIEOR 3106: Fall 2013, Professor Whitt Topics for Discussion: Tuesday, November 19 Alternating Renewal Processes and The Renewal Equation
IEOR 316: Fall 213, Profeor Whitt Topic for Dicuion: Tueday, November 19 Alternating Renewal Procee and The Renewal Equation 1 Alternating Renewal Procee An alternating renewal proce alternate between
More informationName: Solutions Exam 3
Intruction. Anwer each of the quetion on your own paper. Put your name on each page of your paper. Be ure to how your work o that partial credit can be adequately aeed. Credit will not be given for anwer
More informationSIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuits II. Solutions to Assignment 3 February 2005.
SIMON FRASER UNIVERSITY School of Engineering Science ENSC 320 Electric Circuit II Solution to Aignment 3 February 2005. Initial Condition Source 0 V battery witch flip at t 0 find i 3 (t) Component value:
More informationTRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL
GLASNIK MATEMATIČKI Vol. 38583, 73 84 TRIPLE SOLUTIONS FOR THE ONE-DIMENSIONAL p-laplacian Haihen Lü, Donal O Regan and Ravi P. Agarwal Academy of Mathematic and Sytem Science, Beijing, China, National
More informationDigital Control System
Digital Control Sytem Summary # he -tranform play an important role in digital control and dicrete ignal proceing. he -tranform i defined a F () f(k) k () A. Example Conider the following equence: f(k)
More informationLinear System Fundamentals
Linear Sytem Fundamental MEM 355 Performance Enhancement of Dynamical Sytem Harry G. Kwatny Department of Mechanical Engineering & Mechanic Drexel Univerity Content Sytem Repreentation Stability Concept
More informationCHBE320 LECTURE V LAPLACE TRANSFORM AND TRANSFER FUNCTION. Professor Dae Ryook Yang
CHBE3 ECTURE V APACE TRANSFORM AND TRANSFER FUNCTION Profeor Dae Ryook Yang Spring 8 Dept. of Chemical and Biological Engineering 5- Road Map of the ecture V aplace Tranform and Tranfer function Definition
More informationThe Laplace Transform
Chapter 7 The Laplace Tranform 85 In thi chapter we will explore a method for olving linear differential equation with contant coefficient that i widely ued in electrical engineering. It involve the tranformation
More informationBeta Burr XII OR Five Parameter Beta Lomax Distribution: Remarks and Characterizations
Marquette Univerity e-publication@marquette Mathematic, Statitic and Computer Science Faculty Reearch and Publication Mathematic, Statitic and Computer Science, Department of 6-1-2014 Beta Burr XII OR
More informationMulti-dimensional Fuzzy Euler Approximation
Mathematica Aeterna, Vol 7, 2017, no 2, 163-176 Multi-dimenional Fuzzy Euler Approximation Yangyang Hao College of Mathematic and Information Science Hebei Univerity, Baoding 071002, China hdhyywa@163com
More informationANSWERS TO MA1506 TUTORIAL 7. Question 1. (a) We shall use the following s-shifting property: L(f(t)) = F (s) L(e ct f(t)) = F (s c)
ANSWERS O MA56 UORIAL 7 Quetion. a) We hall ue the following -Shifting property: Lft)) = F ) Le ct ft)) = F c) Lt 2 ) = 2 3 ue Ltn ) = n! Lt 2 e 3t ) = Le 3t t 2 ) = n+ 2 + 3) 3 b) Here u denote the Unit
More informationGiven the following circuit with unknown initial capacitor voltage v(0): X(s) Immediately, we know that the transfer function H(s) is
EE 4G Note: Chapter 6 Intructor: Cheung More about ZSR and ZIR. Finding unknown initial condition: Given the following circuit with unknown initial capacitor voltage v0: F v0/ / Input xt 0Ω Output yt -
More informationOne Class of Splitting Iterative Schemes
One Cla of Splitting Iterative Scheme v Ciegi and V. Pakalnytė Vilniu Gedimina Technical Univerity Saulėtekio al. 11, 2054, Vilniu, Lithuania rc@fm.vtu.lt Abtract. Thi paper deal with the tability analyi
More informationInvariance of a Partial Differential Equation of Fractional Order under the Lie Group of Scaling Transformations
JOURNAL OF MATHEMATICAL ANALYSIS AND APPLICATIONS 7, 8197 1998 ARTICLE NO AY986078 Invariance of a Partial Differential Equation of Fractional Order under the Lie Group of Scaling Tranformation Evelyn
More informationTAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES
TAYLOR POLYNOMIALS FOR NABLA DYNAMIC EQUATIONS ON TIME SCALES DOUGLAS R. ANDERSON Abtract. We are concerned with the repreentation of polynomial for nabla dynamic equation on time cale. Once etablihed,
More informationDIFFERENTIAL EQUATIONS
DIFFERENTIAL EQUATIONS Laplace Tranform Paul Dawkin Table of Content Preface... Laplace Tranform... Introduction... The Definition... 5 Laplace Tranform... 9 Invere Laplace Tranform... Step Function...4
More informationPractice Problems - Week #7 Laplace - Step Functions, DE Solutions Solutions
For Quetion -6, rewrite the piecewie function uing tep function, ketch their graph, and find F () = Lf(t). 0 0 < t < 2. f(t) = (t 2 4) 2 < t In tep-function form, f(t) = u 2 (t 2 4) The graph i the olid
More informationChapter 2 Further Properties of the Laplace Transform
Chapter 2 Further Propertie of the Laplace Tranform 2.1 Real Function Sometime, a function F(t) repreent a natural or engineering proce that ha no obviou tarting value. Statitician call thi a time erie.
More informationManprit Kaur and Arun Kumar
CUBIC X-SPLINE INTERPOLATORY FUNCTIONS Manprit Kaur and Arun Kumar manpreet2410@gmail.com, arun04@rediffmail.com Department of Mathematic and Computer Science, R. D. Univerity, Jabalpur, INDIA. Abtract:
More informationSingular perturbation theory
Singular perturbation theory Marc R. Rouel June 21, 2004 1 Introduction When we apply the teady-tate approximation (SSA) in chemical kinetic, we typically argue that ome of the intermediate are highly
More informationA note on the bounds of the error of Gauss Turán-type quadratures
Journal of Computational and Applied Mathematic 2 27 276 282 www.elevier.com/locate/cam A note on the bound of the error of Gau Turán-type quadrature Gradimir V. Milovanović a, Miodrag M. Spalević b, a
More informationPOINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR WEAK SOLUTIONS OF PARABOLIC EQUATIONS
Electronic Journal of Differential Equation, Vol. 206 (206), No. 204, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu POINCARE INEQUALITY AND CAMPANATO ESTIMATES FOR
More informationSOLUTIONS FOR HOMEWORK SECTION 6.4 AND 6.5
SOLUTIONS FOR HOMEWORK SECTION 6.4 AND 6.5 Problem : For each of the following function do the following: (i) Write the function a a piecewie function and ketch it graph, (ii) Write the function a a combination
More informationCorrection for Simple System Example and Notes on Laplace Transforms / Deviation Variables ECHE 550 Fall 2002
Correction for Simple Sytem Example and Note on Laplace Tranform / Deviation Variable ECHE 55 Fall 22 Conider a tank draining from an initial height of h o at time t =. With no flow into the tank (F in
More informationMath 201 Lecture 17: Discontinuous and Periodic Functions
Math 2 Lecture 7: Dicontinuou and Periodic Function Feb. 5, 22 Many example here are taken from the textbook. he firt number in () refer to the problem number in the UA Cutom edition, the econd number
More informationLocal Fractional Laplace s Transform Based Local Fractional Calculus
From the SelectedWork of Xiao-Jun Yang 2 Local Fractional Laplace Tranform Baed Local Fractional Calculu Yang Xiaojun Available at: http://workbeprecom/yang_iaojun/8/ Local Fractional Laplace Tranform
More informationME 375 FINAL EXAM Wednesday, May 6, 2009
ME 375 FINAL EXAM Wedneday, May 6, 9 Diviion Meckl :3 / Adam :3 (circle one) Name_ Intruction () Thi i a cloed book examination, but you are allowed three ingle-ided 8.5 crib heet. A calculator i NOT allowed.
More informationDYNAMIC MODELS FOR CONTROLLER DESIGN
DYNAMIC MODELS FOR CONTROLLER DESIGN M.T. Tham (996,999) Dept. of Chemical and Proce Engineering Newcatle upon Tyne, NE 7RU, UK.. INTRODUCTION The problem of deigning a good control ytem i baically that
More informationA Constraint Propagation Algorithm for Determining the Stability Margin. The paper addresses the stability margin assessment for linear systems
A Contraint Propagation Algorithm for Determining the Stability Margin of Linear Parameter Circuit and Sytem Lubomir Kolev and Simona Filipova-Petrakieva Abtract The paper addree the tability margin aement
More informationCopyright 1967, by the author(s). All rights reserved.
Copyright 1967, by the author(). All right reerved. Permiion to make digital or hard copie of all or part of thi work for peronal or claroom ue i granted without fee provided that copie are not made or
More informationNonlinear Single-Particle Dynamics in High Energy Accelerators
Nonlinear Single-Particle Dynamic in High Energy Accelerator Part 6: Canonical Perturbation Theory Nonlinear Single-Particle Dynamic in High Energy Accelerator Thi coure conit of eight lecture: 1. Introduction
More information18.03SC Final Exam = x 2 y ( ) + x This problem concerns the differential equation. dy 2
803SC Final Exam Thi problem concern the differential equation dy = x y ( ) dx Let y = f (x) be the olution with f ( ) = 0 (a) Sketch the iocline for lope, 0, and, and ketch the direction field along them
More informationTMA4125 Matematikk 4N Spring 2016
Norwegian Univerity of Science and Technology Department of Mathematical Science TMA45 Matematikk 4N Spring 6 Solution to problem et 6 In general, unle ele i noted, if f i a function, then F = L(f denote
More informationChapter 7: The Laplace Transform Part 1
Chapter 7: The Laplace Tranform Part 1 王奕翔 Department of Electrical Engineering National Taiwan Univerity ihwang@ntu.edu.tw November 26, 213 1 / 34 王奕翔 DE Lecture 1 Solving an initial value problem aociated
More informationLaplace Homotopy Analysis Method for Solving Fractional Order Partial Differential Equations
IOSR Journal of Mathematic (IOSR-JM) e-issn: 2278-5728, p-issn: 239-765X. Volume 3, Iue 5 Ver. I (Sep. - Oct. 207), PP 49-54 www.iorjournal.org Laplace Homotopy Analyi Method for Solving Fractional Order
More informationMidterm Test Nov 10, 2010 Student Number:
Mathematic 265 Section: 03 Verion A Full Name: Midterm Tet Nov 0, 200 Student Number: Intruction: There are 6 page in thi tet (including thi cover page).. Caution: There may (or may not) be more than one
More informationThe Riemann Transform
The Riemann Tranform By Armando M. Evangelita Jr. armando78973@gmail.com Augut 28, 28 ABSTRACT In hi 859 paper, Bernhard Riemann ued the integral equation f (x ) x dx to develop an explicit formula for
More informationRepresentation Formulas of Curves in a Two- and Three-Dimensional Lightlike Cone
Reult. Math. 59 (011), 437 451 c 011 Springer Bael AG 14-6383/11/030437-15 publihed online April, 011 DOI 10.1007/0005-011-0108-y Reult in Mathematic Repreentation Formula of Curve in a Two- and Three-Dimenional
More informationCHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS
CHAPTER 8 OBSERVER BASED REDUCED ORDER CONTROLLER DESIGN FOR LARGE SCALE LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.1 INTRODUCTION 8.2 REDUCED ORDER MODEL DESIGN FOR LINEAR DISCRETE-TIME CONTROL SYSTEMS 8.3
More information6. KALMAN-BUCY FILTER
6. KALMAN-BUCY FILTER 6.1. Motivation and preliminary. A wa hown in Lecture 2, the optimal control i a function of all coordinate of controlled proce. Very often, it i not impoible to oberve a controlled
More informationDIFFERENTIAL EQUATIONS Laplace Transforms. Paul Dawkins
DIFFERENTIAL EQUATIONS Laplace Tranform Paul Dawkin Table of Content Preface... Laplace Tranform... Introduction... The Definition... 5 Laplace Tranform... 9 Invere Laplace Tranform... Step Function...
More informationinto a discrete time function. Recall that the table of Laplace/z-transforms is constructed by (i) selecting to get
Lecture 25 Introduction to Some Matlab c2d Code in Relation to Sampled Sytem here are many way to convert a continuou time function, { h( t) ; t [0, )} into a dicrete time function { h ( k) ; k {0,,, }}
More informationComplex Inversion Formula for Stieltjes and Widder Transforms with Applications
Int. J. Contemp. Math. Sciences, Vol. 3, 8, no. 16, 761-77 Complex Inversion Formula for Stieltjes and Widder Transforms with Applications A. Aghili and A. Ansari Department of Mathematics, Faculty of
More informationFOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS
FOURIER SERIES AND PERIODIC SOLUTIONS OF DIFFERENTIAL EQUATIONS Nguyen Thanh Lan Department of Mathematic Wetern Kentucky Univerity Email: lan.nguyen@wku.edu ABSTRACT: We ue Fourier erie to find a neceary
More informationR L R L L sl C L 1 sc
2260 N. Cotter PRACTICE FINAL EXAM SOLUTION: Prob 3 3. (50 point) u(t) V i(t) L - R v(t) C - The initial energy tored in the circuit i zero. 500 Ω L 200 mh a. Chooe value of R and C to accomplih the following:
More informationwhere F (x) (called the Similarity Factor (SF)) denotes the function
italian journal of pure and applied mathematic n. 33 014 15 34) 15 GENERALIZED EXPONENTIAL OPERATORS AND DIFFERENCE EQUATIONS Mohammad Aif 1 Anju Gupta Department of Mathematic Kalindi College Univerity
More informationMath Skills. Scientific Notation. Uncertainty in Measurements. Appendix A5 SKILLS HANDBOOK
ppendix 5 Scientific Notation It i difficult to work with very large or very mall number when they are written in common decimal notation. Uually it i poible to accommodate uch number by changing the SI
More informationProblem 1 (4 5 points)
ACM95/b Problem Set 3 Solution /7/4 Problem (4 5 point) The following (trivial once you 'get it') problem i deigned to help thoe of you who had trouble with Problem Set ' problem 7c. It will alo help you
More informationin a circular cylindrical cavity K. Kakazu Department of Physics, University of the Ryukyus, Okinawa , Japan Y. S. Kim
Quantization of electromagnetic eld in a circular cylindrical cavity K. Kakazu Department of Phyic, Univerity of the Ryukyu, Okinawa 903-0, Japan Y. S. Kim Department of Phyic, Univerity of Maryland, College
More informationAn analysis of the temperature field of the workpiece in dry continuous grinding
J Eng Math (21 67:165 174 DOI 1.17/1665-9-9335-6 An analyi of the temperature field of the workpiece in dry continuou grinding J. L. González Santander J. Pérez P. Fernández de Córdoba J. M. Iidro Received:
More informationName: Solutions Exam 2
Name: Solution Exam Intruction. Anwer each of the quetion on your own paper. Put your name on each page of your paper. Be ure to how your work o that partial credit can be adequately aeed. Credit will
More informationControl Systems Analysis and Design by the Root-Locus Method
6 Control Sytem Analyi and Deign by the Root-Locu Method 6 1 INTRODUCTION The baic characteritic of the tranient repone of a cloed-loop ytem i cloely related to the location of the cloed-loop pole. If
More informationProblem 1. Construct a filtered probability space on which a Brownian motion W and an adapted process X are defined and such that
Stochatic Calculu Example heet 4 - Lent 5 Michael Tehranchi Problem. Contruct a filtered probability pace on which a Brownian motion W and an adapted proce X are defined and uch that dx t = X t t dt +
More informationSTABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE DELAYS
Bulletin of Mathematical Analyi and Application ISSN: 1821-1291, URL: http://bmathaa.org Volume 1 Iue 2(218), Page 19-3. STABILITY OF A LINEAR INTEGRO-DIFFERENTIAL EQUATION OF FIRST ORDER WITH VARIABLE
More informationSocial Studies 201 Notes for November 14, 2003
1 Social Studie 201 Note for November 14, 2003 Etimation of a mean, mall ample ize Section 8.4, p. 501. When a reearcher ha only a mall ample ize available, the central limit theorem doe not apply to the
More informationEE Control Systems LECTURE 6
Copyright FL Lewi 999 All right reerved EE - Control Sytem LECTURE 6 Updated: Sunday, February, 999 BLOCK DIAGRAM AND MASON'S FORMULA A linear time-invariant (LTI) ytem can be repreented in many way, including:
More informationLecture 2: The z-transform
5-59- Control Sytem II FS 28 Lecture 2: The -Tranform From the Laplace Tranform to the tranform The Laplace tranform i an integral tranform which take a function of a real variable t to a function of a
More informationMA 266 FINAL EXAM INSTRUCTIONS May 2, 2005
MA 66 FINAL EXAM INSTRUCTIONS May, 5 NAME INSTRUCTOR. You mut ue a # pencil on the mark ene heet anwer heet.. If the cover of your quetion booklet i GREEN, write in the TEST/QUIZ NUMBER boxe and blacken
More information696 Fu Jing-Li et al Vol. 12 form in generalized coordinate Q ffiq dt = 0 ( = 1; ;n): (3) For nonholonomic ytem, ffiq are not independent of
Vol 12 No 7, July 2003 cfl 2003 Chin. Phy. Soc. 1009-1963/2003/12(07)/0695-05 Chinee Phyic and IOP Publihing Ltd Lie ymmetrie and conerved quantitie of controllable nonholonomic dynamical ytem Fu Jing-Li(ΛΠ±)
More informationComputers and Mathematics with Applications. Sharp algebraic periodicity conditions for linear higher order
Computer and Mathematic with Application 64 (2012) 2262 2274 Content lit available at SciVere ScienceDirect Computer and Mathematic with Application journal homepage: wwweleviercom/locate/camwa Sharp algebraic
More informationNULL HELIX AND k-type NULL SLANT HELICES IN E 4 1
REVISTA DE LA UNIÓN MATEMÁTICA ARGENTINA Vol. 57, No. 1, 2016, Page 71 83 Publihed online: March 3, 2016 NULL HELIX AND k-type NULL SLANT HELICES IN E 4 1 JINHUA QIAN AND YOUNG HO KIM Abtract. We tudy
More informationWhat lies between Δx E, which represents the steam valve, and ΔP M, which is the mechanical power into the synchronous machine?
A 2.0 Introduction In the lat et of note, we developed a model of the peed governing mechanim, which i given below: xˆ K ( Pˆ ˆ) E () In thee note, we want to extend thi model o that it relate the actual
More informationChapter 7: The Laplace Transform
Chapter 7: The Laplace Tranform 王奕翔 Department of Electrical Engineering National Taiwan Univerity ihwang@ntu.edu.tw November 2, 213 1 / 25 王奕翔 DE Lecture 1 Solving an initial value problem aociated with
More information1 Routh Array: 15 points
EE C28 / ME34 Problem Set 3 Solution Fall 2 Routh Array: 5 point Conider the ytem below, with D() k(+), w(t), G() +2, and H y() 2 ++2 2(+). Find the cloed loop tranfer function Y () R(), and range of k
More informationThermal Stress in a Half-Space with Mixed Boundary Conditions due to Time Dependent Heat Source
IOSR Journal of Mathematic (IOSR-JM) e-issn: 2278-5728, p-issn: 239-765X Volume, Iue 6 Ver V (Nov - Dec 205), PP 9-25 wwwiorjournalorg Thermal Stre in a Half-Space with Mixed Boundary Condition due to
More informationRiemann s Functional Equation is Not a Valid Function and Its Implication on the Riemann Hypothesis. Armando M. Evangelista Jr.
Riemann Functional Equation i Not a Valid Function and It Implication on the Riemann Hypothei By Armando M. Evangelita Jr. armando78973@gmail.com On Augut 28, 28 ABSTRACT Riemann functional equation wa
More informationThe continuous time random walk (CTRW) was introduced by Montroll and Weiss 1.
1 I. CONTINUOUS TIME RANDOM WALK The continuou time random walk (CTRW) wa introduced by Montroll and Wei 1. Unlike dicrete time random walk treated o far, in the CTRW the number of jump n made by the walker
More informationLAPLACE TRANSFORM REVIEW SOLUTIONS
LAPLACE TRANSFORM REVIEW SOLUTIONS. Find the Laplace tranform for the following function. If an image i given, firt write out the function and then take the tranform. a e t inh4t From #8 on the table:
More informationSolutions for homework 8
Solution for homework 8 Section. Baic propertie of the Laplace Tranform. Ue the linearity of the Laplace tranform (Propoition.7) and Table of Laplace tranform on page 04 to find the Laplace tranform of
More information8. [12 Points] Find a particular solution of the differential equation. t 2 y + ty 4y = t 3, y h = c 1 t 2 + c 2 t 2.
Intruction. Anwer each of the quetion on your own paper. Put your name on each page of your paper. Be ure to how your work o that partial credit can be adequately aeed. Credit will not be given for anwer
More informationGeneral System of Nonconvex Variational Inequalities and Parallel Projection Method
Mathematica Moravica Vol. 16-2 (2012), 79 87 General Sytem of Nonconvex Variational Inequalitie and Parallel Projection Method Balwant Singh Thakur and Suja Varghee Abtract. Uing the prox-regularity notion,
More informationConvergence criteria and optimization techniques for beam moments
Pure Appl. Opt. 7 (1998) 1221 1230. Printed in the UK PII: S0963-9659(98)90684-5 Convergence criteria and optimization technique for beam moment G Gbur and P S Carney Department of Phyic and Atronomy and
More informationSome Sets of GCF ϵ Expansions Whose Parameter ϵ Fetch the Marginal Value
Journal of Mathematical Reearch with Application May, 205, Vol 35, No 3, pp 256 262 DOI:03770/jin:2095-26520503002 Http://jmredluteducn Some Set of GCF ϵ Expanion Whoe Parameter ϵ Fetch the Marginal Value
More informationA Simplified Methodology for the Synthesis of Adaptive Flight Control Systems
A Simplified Methodology for the Synthei of Adaptive Flight Control Sytem J.ROUSHANIAN, F.NADJAFI Department of Mechanical Engineering KNT Univerity of Technology 3Mirdamad St. Tehran IRAN Abtract- A implified
More informationThe Hassenpflug Matrix Tensor Notation
The Haenpflug Matrix Tenor Notation D.N.J. El Dept of Mech Mechatron Eng Univ of Stellenboch, South Africa e-mail: dnjel@un.ac.za 2009/09/01 Abtract Thi i a ample document to illutrate the typeetting of
More informationLTV System Modelling
Helinki Univerit of Technolog S-72.333 Potgraduate Coure in Radiocommunication Fall 2000 LTV Stem Modelling Heikki Lorentz Sonera Entrum O heikki.lorentz@onera.fi Januar 23 rd 200 Content. Introduction
More informationMath 334 Fall 2011 Homework 10 Solutions
Nov. 5, Math 334 Fall Homework Solution Baic Problem. Expre the following function uing the unit tep function. And ketch their graph. < t < a g(t = < t < t > t t < b g(t = t Solution. a We
More informationChapter 13. Root Locus Introduction
Chapter 13 Root Locu 13.1 Introduction In the previou chapter we had a glimpe of controller deign iue through ome imple example. Obviouly when we have higher order ytem, uch imple deign technique will
More informationLecture 3. January 9, 2018
Lecture 3 January 9, 208 Some complex analyi Although you might have never taken a complex analyi coure, you perhap till know what a complex number i. It i a number of the form z = x + iy, where x and
More information(3) A bilinear map B : S(R n ) S(R m ) B is continuous (for the product topology) if and only if there exist C, N and M such that
The material here can be found in Hörmander Volume 1, Chapter VII but he ha already done almot all of ditribution theory by thi point(!) Johi and Friedlander Chapter 8. Recall that S( ) i a complete metric
More informationSOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR
Kragujevac Journal of Mathematic Volume 4 08 Page 87 97. SOME MONOTONICITY PROPERTIES AND INEQUALITIES FOR THE p k-gamma FUNCTION KWARA NANTOMAH FATON MEROVCI AND SULEMAN NASIRU 3 Abtract. In thi paper
More informationLaplace Transform. Chapter 8. Contents
Chapter 8 Laplace Tranform Content 8.1 Introduction to the Laplace Method..... 443 8.2 Laplace Integral Table............. 45 8.3 Laplace Tranform Rule............ 456 8.4 Heaviide Method...............
More informationINITIAL-VALUE PROBLEMS FOR HYBRID HADAMARD FRACTIONAL DIFFERENTIAL EQUATIONS
Electronic Journal of Differential Equation, Vol. 204 204, No. 6, pp. 8. ISSN: 072-669. URL: http://ejde.math.txtate.edu or http://ejde.math.unt.edu ftp ejde.math.txtate.edu INITIAL-VALUE PROBLEMS FOR
More information